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Predicting the Cosmological Constant from the Causal Entropic Principle

High Energy Physics - Theory · Submitted 15 Feb 2007 · 59 references

Pith's verdict: The real content is the entropy-source computation and the t_edge = t_peak matching, not the principle; the calculation is competent and the soft spots are the ones the authors themselves flag.

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arXiv IDhep-th/0702115 (version 3)
Pith ID3XDXX7GY, Pith's permanent record of this paper and its review
CitationGilad Perez, Graham D. Kribs, Raphael Bousso, Roni Harnik. "Predicting the Cosmological Constant from the Causal Entropic Principle." arXiv:hep-th/0702115 (2007). https://pith.science/paper/3XDXX7GY
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The paper

The paper claims

Weighting vacua by entropy production in the causal diamond yields a distribution for the cosmological constant whose 1-sigma band contains the observed value.

The reading

The cosmological constant is about 10^123 times smaller than naive particle physics estimates. One response is to treat it as an environmental variable: different regions of a multiverse have different values, and we should ask which values observers are likely to see. The standard anthropic approach assumes observers need galaxies, which caps the value but leaves the observed one looking unlikely. This paper proposes a different weight. Any observation requires free energy and produces entropy, so the authors conjecture that the number of observations in a region scales with the total entropy produced there. They also restrict to the causal diamond, the largest spacetime region a single observer can probe. A smaller cosmological constant means a larger diamond and more time before vacuum domination, so small values get a compensating bonus. The authors then estimate entropy production in our universe. They find it is dominated by infrared photons from dust heated by starlight, peaking 2 to 3.5 billion years after the big bang. Combining this rate with the diamond volume gives a probability distribution over the cosmological constant. The distribution peaks where the diamond's edge time matches the entropy production peak, which is close to the observed value. The observed value sits inside the 1-sigma band for both star formation histories they try. The catch is that the star formation history is measured in our universe, which already has the observed cosmological constant. The authors argue the peak time is set by astrophysics in the matter era and is therefore independent of the cosmological constant, but this is an assumption. The result is best read as a consistency check on a subspace of the landscape, not a parameter-free prediction.
Extended reading notes

Core claim

The probability distribution dP/d log rho_Lambda proportional to rho_Lambda times Delta S(rho_Lambda), with Delta S the total matter entropy produced in the causal diamond, peaks near log rho_Lambda approximately -123 and places the observed value (1.25 x 10^-123) inside the 1-sigma band for both star formation histories considered (Fig. 8).

Load-bearing premise

The star formation rate history, in particular its peak time t_peak approximately 2 to 3 Gyr, is independent of rho_Lambda and can be imported from observations of our own universe. This enters at Section 3.3 (Eq. 3.23 and surrounding text), where the authors write that the peak is still in the matter dominated era and that the cosmological constant played no dynamical role and cannot have anything to do with this peak. If the SFR peak time shifted with rho_Lambda, the predicted peak of dP/d log rho_Lambda would shift with it.

Original abstract

We compute the expected value of the cosmological constant in our universe from the Causal Entropic Principle. Since observers must obey the laws of thermodynamics and causality, the principle asserts that physical parameters are most likely to be found in the range of values for which the total entropy production within a causally connected region is maximized. Despite the absence of more explicit anthropic criteria, the resulting probability distribution turns out to be in excellent agreement with observation. In particular, we find that dust heated by stars dominates the entropy production, demonstrating the remarkable power of this thermodynamic selection criterion. The alternative approach - weighting by the number of "observers per baryon" - is less well-defined, requires problematic assumptions about the nature of observers, and yet prefers values larger than present experimental bounds.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,316 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.20 · human participants 0.02 · controlled comparison 0.15 · randomized assignment 0.01 · states quantitative result 0.18 · compares with prior results 0.94 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v3. Results and the main claim are underlined; .

We compute the expected value of the cosmological constant in our universe from the Causal Entropic Principle. Since observers must obey the laws of thermodynamics and causality, the principle asserts that physical parameters are most likely to be found in the range of values for which the total entropy production within a causally connected region is maximized. Despite the absence of more explicit anthropic criteria, the resulting probability distribution turns out to be in excellent agreement with observation. In particular, we find that dust heated by stars dominates the entropy production, demonstrating the remarkable power of this thermodynamic selection criterion. The alternative approach - weighting by the number of "observers per baryon" - is less well-defined, requires problematic assumptions about the nature of observers, and yet prefers values larger than present experimental bounds.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We compute the expected value of the cosmological constant in our universe from the Causal Entropic Principle. contribution 0.99 0.96 0.20 asserted 0.97
s1 Since observers must obey the laws of thermodynamics and causality, the principle asserts that physical parameters are most likely to be found in the range of values for which the total entropy production within a causally connected region is maximized. background 0.50 0.11 0.07 asserted 0.97
s2 Despite the absence of more explicit anthropic criteria, the resulting probability distribution turns out to be in excellent agreement with observation. result 0.94 0.88 0.54 asserted 0.97
s3 In particular, we find that dust heated by stars dominates the entropy production, demonstrating the remarkable power of this thermodynamic selection criterion. result 0.72 0.94 0.19 asserted 1.00
s4 The alternative approach - weighting by the number of "observers per baryon" - is less well-defined, requires problematic assumptions about the nature of observers, and yet prefers values larger than present experimental bounds. result 0.46 0.37 0.05 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.97 · evidence from simulation or computation 0.83.

What was examined, and what was not

sources read
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  • figures and tables
  • references and citing sentences
  • relations to other papers
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not run
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  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

Figures
Figure 1. The probability distribution of the vacuum energy measured by typical observers, computed from the Causal Entropic Principle, is shown as a solid curve. The values consistent with present cosmological data, in the shaded vertical bar, are well inside the 1σ region (shown in white), and hence, not atypical. For comparison, the dashed line shows the distribution derived by estimating the number of observers per baryon. Unlike our curve, it assumes that galaxies are necessary for observers; yet, the observed value is very unlikely under this distribution. For more details about both…
Figure 2. Weighted by “observers per baryon”, the probability distribution for ρΛ de￾pends strongly on specific assumptions about conditions necessary for life. Three curves are shown, corresponding to different choices for the minimum required mass of a galaxy: M∗ = (107 , 109 , 1012)M⊙. In neither case is the observed value (vertical bar) in the preferred range. The choice M∗ = 107M⊙ (also shown in
Figure 3. A causal diamond is the largest spacetime region over which matter can interact. It is delimited by a future lightcone from a point on the reheating surface (orange/light), and by a past lightcone from a late-time event (blue/dark); in the case of de Sitter vacua this is the cosmological horizon. A vacuum should be weighted by the number of observations made in this spacetime region. Since observation requires free energy, we expect that on average, this number will be proportional to the amount of entropy, ∆S, produced in the causal diamond. Entropy entering through the bottom cone…
Figure 4. The lower plot shows comoving volume in the causal diamond, Vc, as a function of time for ρΛ = (0.1, 1, 10) times the observed value given in Eq. (1.1). The kink in the comoving volume corresponds to the “edge” of the causal diamond, where the top and bottom cone meet (see
Figure 5. The star formation rate as a function of time from Nagamine et al. [56], labeled “N”, and from Hopkins and Beacom [57], labeled “H”. They are peaked at t⋆ ∼1.7 Gyr and 2.8 Gyr respectively. We have normalized both SFRs such that the stellar luminosity density calculated below agrees with the bolometric luminosity observed today. It should be noted, however, that our result is not sensitive to this re-normalization. Both SFRs are shown in
Figure 6. The entropy production rate in our universe as a function of time, from dust heated by starlight. The two curves shown correspond to different models of the star formation history of the universe [56, 57]; see
Figure 7. The entropy production rate of
Figure 8. The probability distribution over log(ρΛ) computed from the Causal Entropic Principle. The two curves shown arise from two different models of the star formation rate (see Figs. 5 and 6). Their differences hint at the systematic uncertainties in our calculation that arise since the history of entropy production is not known to arbitrary precision. These uncertainties are apparently irrelevant to our main conclusion: either way, the observed value of ρΛ (vertical bar) is not unlikely. the Hopkins et al. SFR, we find the median value ρΛ = 2.1 × 10−123 with the 1σ error band between…
Figure 9. This cartoon demonstrates how the Causal Entropic Principle leads to a pre￾ferred value of the cosmological constant. The horizontal band represents the rate of entropy production; darker areas correspond to a higher rate. Vacua are weighted by ∆S, the total amount of “darkness” inside a causal diamond. Vacua with large cosmological constant are plentiful in the landscape, but they lead to small causal diamonds, which capture virtually no entropy production (right). For some smaller value, the diamond will be just large enough to capture the bulk of the entropy production (center).…

Figures reproduced from arXiv:hep-th/0702115 by the authors.

References
How the literature uses it

50 arXiv papers cite this in 140 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 87 sentences without a confident label

Builds on it 2 papers
Uses its method or tool 6 papers
Uses its data or values 2 papers
Compares with it 7 papers
Cites it as support 2 papers
  • As shown in Ref. [ref] , the CIB represents the dominant portion of the entropy produced in our universe within the causal diamond.

    The Entropic Landscape · Comparison with observation · 0.99

  • As shown in the appendix of [ref] , this is a reasonable model of our universe, and ignoring the radiation era introduces only a negligible error.

    Replacing Anthropy with entropy: Does it work? · Entropy and inflation · 0.99

Cites it as background 22 papers
  • Bousso et al. [ref] proposed the causal entropic principle (CEP), an elegant approach which weighs different parameter choices according to entropy production in the corresponding cosmology.

    Dark Matter Annihilations in the Causal Diamond · Introduction · 0.91

  • Here, we consider two closely related but inequivalent members of the surviving group of measures: the causal diamond cut-off [ref] and the causal patch cut-off [ref] .

    Predictions from Star Formation in the Multiverse · Introduction · 0.84

  • Recently, it was proposed [ref] that the correct anthropic measure for the probability of observing a given universe is tied to the amount of entropy production in that universe.

    Replacing Anthropy with entropy: Does it work? · Introduction · 0.82

Discussion

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